Anomalous bathymetry, 3D edge driven convection, and dynamic topography at the western Atlantic passive margin
Research highlights
▶ Edge driven convection inducing offshore uplift and near margin deepening. ▶ Along strike variation of topography/bathymetry attributed to sub-lithospheric flow. ▶ Onshore topographic lows may be related to western Atlantic sedimentary basins. ▶ Additional possible interpretation of negative dynamic topography in Conrad et al. (2004).
Introduction
Oceanic lithosphere exhibits a consistent and well-understood increase in bathymetry from mid-ocean ridges to passive continental margins (Turcotte and Schubert, 2002). However, the plates also contain more enigmatic, shorter wavelength bathymetric features superimposed on the plate cooling and subsidence phenomenon. Some of these features may be caused by the relative motion of the ocean plate over hot spots, resulting in a track of elevated seamounts parallel to the direction of the plate motion (e.g., Wilson, 1963). The topographic anomalies can also be caused by various processes such as seafloor volcanism, post-rift epeirogeny (Conrad et al., 2004), and flexural loading, but this contribution focuses on the possibility that some of the bathymetric features (or at least some component of their anomalous bathymetry) are a manifestation of dynamic topography. Dynamic topography is defined as vertical motions of the surface caused by imposed normal stresses at the base of the lithosphere from underlying mantle flow (McKenzie, 1977, Cazenave et al., 1989, Kido and Seno, 1994).
At a passive continent–ocean margin, a sharp lateral variation in thermal structure of the lithosphere may induce the formation of a convective mantle fluid flow (Elder, 1976). This style of convection was studied by King and Anderson (1995) as a process to account for the formation of flood basalts near the margins of cratonic lithosphere. The term “edge driven convection” (EDC) was put forward to denote such a regime of mantle convection induced by the sharp lateral thermal gradient as a continent–ocean boundary (King and Anderson, 1998). The thermal discontinuity can initiate a small-scale mantle convection cell with downwelling at the continental margin and corresponding upwelling further offshore. Ritsema et al. (1999) and King and Ritsema (2000) infer that velocity anomalies in the upper mantle in the tomographic model S20RTS delineate the thermal anomalies of edge driven convective flow along portions of eastern North America, western Africa and eastern South America. They put forward EDC as an explanation for intraplate African and South American hotspot volcanism (Ritsema et al., 1999, King and Ritsema, 2000, King, 2007).
A prominent group of bathymetric and thermal anomalies exists in the western Atlantic adjacent to the passive continent–ocean margin. Vogt (1991) put forward several reasons why several of these specific topographic swell patterns (including the Bermuda Rise) could not be reconciled with simple hot spot theory. Firstly, the lack of volcanism on or in the vicinity of Bermuda during the past 33 Myr precludes an active mantle plume source for supporting the topography. Secondly, the orientation of the Bermuda Rise is almost orthogonal to the predicted fixed hot spot track associated with North American plate motion. Vogt (1991) suggested that these anomalous topographic features may be produced by a thermal instability traveling with the North American plate rather than a deep mantle plume. That is, a process akin to the subsequently proposed edge driven convection (King and Anderson, 1995).
Edge driven convection (EDC) within the upper mantle produces a topographic perturbation that may be consistent with bathymetric perturbations at a passive plate boundary (King and Anderson, 1998). Two-dimensional modeling shows that such EDC induces subsidence at the continental margin and an offshore peak/plateau of high topography on the ocean plate (Shahnas and Pysklywec, 2004). Conrad et al. (2004) proposed that the downgoing portion of a potential edge driven mantle convection cell may cause an anomalously deep region off the coast of Nova Scotia. Unlike a hot spot, the edge driven convection cell and associated topography migrate with moving surface plates. As a result, EDC-related topography on the seafloor would not show a track of bathymetry, but rather would develop in a quasi-stable geographic location. The amplitude and wavelength of the dynamic topography could vary in time, especially in the presence of a simulated surface plate motion (Shahnas and Pysklywec, 2004). However, the two-dimensional models did not give any insight into how the flow/topographic features varied in the direction parallel to the strike of the passive plate boundary.
The purpose of this work is to consider the variation of topography along the eastern seaboard of North America and the three-dimensional (3D) nature of EDC. A 3D examination may be important in our understanding of this small-scale convective phenomenon. The investigation extends the previous 2D studies by determining the anomalous bathymetry/topography at a number of profiles along the passive margin of the continent. Further, 3D geodynamic computational experiments are executed to model the edge driven mantle flow and associated surface topographic features, or lack thereof, in the 3D geodynamic models. The long-wavelength topographic/bathymetric anomalies of the region are considered to be dynamic topography associated with EDC. Taken into primary consideration are the stability and longevity of the continental margin and the imposed viscosity structure of the ocean–continent lithosphere (Shapiro et al., 1999).
In this study, the focus is on the topographic expression of mantle convection and the observed topographic anomalies. It is recognized that there exists a thermal expression and thermal anomalies of the edge driven convection as well. Certainly, magmatic features of Bermuda and the Bermuda Rise are prominent and are transient in nature (Vogt, 1991, Harris and McNutt, 2007). Furthermore, thermal alteration of the ocean plate due to these magmatic effects may contribute to topography anomalies but this is not considered here.
Section snippets
Anomalous topography in the western North Atlantic
Various data have been compiled to demonstrate the anomalous bathymetry/topography across the western part of the North Atlantic and Eastern seaboard of North America. The first set is shown as a series of profiles approximately perpendicular to the continental margin (Fig. 1). These bathymetric anomalies were derived by correcting the observed seafloor bathymetry for cooling and subsidence of the ocean plate away from the mid-Atlantic ridge and isostatic sediment loading. Two sources of data
Numerical model theory and design
The computational experiments were designed as upper mantle scale models of an idealized continent–ocean passive margin. The passive margin is emplaced as a step-function in thermal and rheological properties of a model continental and oceanic lithosphere (Fig. 3). The implemented approach is adopted from Shahnas and Pysklywec (2004), King and Anderson (1998), and Shapiro et al. (1999).
The experiments are conducted using a finite element thermal convection code CitcomS version 1.1 (Zhong et
Modeling results
Among a series of experiment runs, the results from representative models to illustrate the flow patterns and associated topography in the 3D system are presented. Using these select experiment runs, we show how the nature of the 3D edge driven convection is modified with changes to the initial thermal structure along-strike to the model plate margin.
Discussion/conclusion
The residual bathymetry and topography in the western North Atlantic are shown to consist of a deepening near the ocean–continent margin and uplift offshore. Two independent data sets show the same patterns, with amplitudes to this residual topography reaching ∼1000s of metres. While there are variations to this residual bathymetry along-strike to the margin, such variations are second-order compared with the conjugate deepening-uplift perpendicular to the margin. The 3D experiments depict
Acknowledgements
I would like to thank Dr. Russell Pysklywec for his guidance and support during the completion of this work; Dr. M. Hosein Shahnas for his assistance with developing the initial temperature profiles for the simulations; as well as my wife Michelle and mother Annette for their support and review of this manuscript. This work has been funded by the NSERC Discovery Grant.
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